In this study, the mechanical load on a bullet-shaped indenter when impacted by a single-ply Kevlar fabric was experimentally investigated using a reverse ballistics method at both quasi-static and dynamic rates. Different indenter geometries, namely the 9-mm Luger, .223 Remington, and .308 Winchester bullet geometries, were used. The penetration load of the stationary indenter was measured using a force transducer located behind the indenter, and the penetration load was then plotted against the impact velocity of the fabric sample. Different mechanisms of penetration were observed at different impact velocities. Penetration mechanisms were also found to be highly dependent on projectile nose geometry. A modified method to obtain an approximate ballistic limit based on the impact loads was used to compare the efficacy of different geometry types.The capability of a bullet-resistant ballistic fabric in stopping a projectile (typically measured using the V50 ballistic limit) during impact is dependent on several mechanisms, such as fiber and fabric mechanical properties (e.g. density and tensile modulus), fabric weave structure, far-field boundary conditions, and projectile geometry. The energy-absorption mechanism of the fabric is dependent on the projectile striking velocity. Below the ballistic limit, there is limited to no penetration, implying that the striking velocities below that limit have zero residual velocity. Past the ballistic limit, the residual velocity is typically observed to increase rapidly for a small range of velocities before increasing relatively linearly with respect to the striking velocity at high velocities. 1 The change in residual velocity behavior across the whole range of velocities indicates a possible change in failure modes and energy-absorption mechanisms. In particular, previous studies have shown that at high velocities, the only dominant energy-dissipation mechanism is via tensile loading of the yarn. 2,3 Previous studies by Cunniff 3,4 and Hudspeth et al. 5 have shown that the effect of aperture size is negligible above the V50 limit, indicating that the damage done at high-impact velocities tends to be localized. On the other hand, at velocities below the V50 limit, mechanisms such as inter-yarn friction, yarn-projectile friction, etc., tend to play a part in dissipating energy as well, and these mechanisms involve a much larger zone of impact. The projectile geometry, in any case, accounts for differences in fabric ballistic performance, 5 which is the reason destructive testing of bullet-resistant vests is dependent on bullet type and threat level.The typical energy-absorption curve is characteristically m-shaped, that is, the energy-absorption increases with striking velocity up to the V50 limit before decreasing for a range of velocities. Past the V50, the kinetic energy absorbed by the fabric system is calculated by subtracting the residual kinetic energy from the